The content in this site are as follows : From Spins to Fields,
The Ising Model, Landau Mean Field Theory, Universality, Critical
Exponents, Landau-Ginzburg Theory, Domain Walls, The Lower Critical Dimension,
My First Path Integral, The Thermodynamic Free Energy (again); Correlation
Functions, Correlation Length; The Upper Critical Dimension, The Analogy with
Quantum Field Theory, The Renormalisation Group, The Big Idea, Universality
Explained, Scaling Explained; Relevant, Irrelevant and Marginal; The Gaussian
Fixed Point, Dangerously Irrelevant Operators, Interactions, Feynman Diagrams;
the Epsilon Expansion, the Wilson-Fisher Fixed Point, A Sniff of Conformal
Symmetry, Continuous Symmetry, The Importance of Symmetry, O(N) Models,
Goldstone Bosons and Goldstone's Theorem, The Mermin-Wagner Theorem; Sigma
Models, Background Fields, Large N, the Kosterlitz-Thouless Transition,
Vortices, the Coulomb Gas, the Sine-Gordon Model, RG for KT and SG.
This PDF book covers the
following topics related to Non-equilibrium Quantum Field Theory : Fundamentals
of Nonequilibrium Statistical Mechanics, Basics of Nonequilibrium Quantum Field
Theory, Gauge Invariance, Dissipation, Entropy, Noise and Decoherence, Thermal,
Kinetic and Hydrodynamic Regimes, Applications to Selected Current Research.
Author(s): Esteban A. Calzetta, University of Buenos Aires
and Conicet, Bei-lok B. Hu, University of Maryland
This book
online covers the following topics related to Introduction to Gauge Field Theory
: Path integrals, Path integrals in non-relativistic quantum mechanics,
Classical field theory, Quantum field theory of a scalar field, Scattering
amplitudes, Feynman rules for kcp* theory, Renormalisation of X(p4 theory,
Quantum field theory with fermions, Gauge field theories, Feynman rules for
quantum chromodynamics, Renormalisation of q c d and q e d at one-loop order, q
c d and asymptotic freedom, Spontaneous symmetry breaking, Feynman rules for
electroweak theory, Renormalisation of electroweak theory, Grand unified theory,
Field theories at finite temperature.